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Search: Author = T.Zhao

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2023MA04      Phys.Rev. C 107, 014310 (2023)

N.-N.Ma, Ti.-L.Zhao, W.-Xi.Wang, H.-F.Zhang

Simple deep-learning approach for α-decay half-life studies

RADIOACTIVITY N=90-180(α); A=160-320(α); Z=80-120(α); calculated T_1/2. The deep learning algorithm trained directly with sets of experimental α-decay half-lives.

doi: 10.1103/PhysRevC.107.014310
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2023ZH22      J.Phys.(London) G50, 045101 (2023)

T.L.Zhao, X.J.Bao, H.F.Zhang

Effect of deformation dependence and mirror nucleus corrections energy on multinucleon transfer reaction cross sections

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=450 MeV; ²³⁸U(⁶⁴Ni, X), E(cm)=307.40 MeV; calculated σ using the dinuclear system (DNS) model, three macroscopic microscopic mass models. Comparison with available data.

doi: 10.1088/1361-6471/acb4b2
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2023ZH41      Phys.Rev. C 108, 024602 (2023)

T.L.Zhao, X.J.Bao, H.F.Zhang

Exploring the optimal way to produce Z=100-106 neutron-rich nuclei

NUCLEAR REACTIONS ²³⁸U(¹⁶O, X), E(cm)=70-160 MeV; calculated capture σ(E). ²⁴⁸Cm(¹⁸O, 4n), E^*=28-60 MeV;²⁴⁸Cm(¹⁸O, 5n), E^*=40-60 MeV;²⁴⁸Cm(¹⁸O, 6n), E^*=46-60 MeV;²⁴⁴Pu(²²Ne, 5n), E^*=40-56 MeV; calculated evaporation residue σ(E). ²⁴⁸Cm(²³⁸U, X)²³⁹Bk/²⁴⁰Bk/²⁴¹Bk/²⁴²Bk/²⁴³Bk/²⁴⁴Bk/²⁴⁵Bk/²⁴⁶Bk/²⁴⁷Bk/²⁴⁸Bk/²⁴⁹Bk/²⁵⁰Bk/²⁵¹Bk/²⁵²Bk/²⁵³Bk/²⁵⁴Bk/²⁵⁵Bk/²⁵⁶Bk/²⁵⁷Bk/²⁵⁸Bk/²⁵⁹Bk/²⁶⁰Bk/²⁴⁰Cf/²⁴¹Cf/²⁴²Cf/²⁴³Cf/²⁴⁴Cf/²⁴⁵Cf/²⁴⁶Cf/²⁴⁷Cf/²⁴⁸Cf/²⁴⁹Cf/²⁵⁰Cf/²⁵¹Cf/²⁵²Cf/²⁵³Cf/²⁵⁴Cf/²⁵⁵Cf/²⁵⁶Cf/²⁵⁷Cf/²⁵⁸Cf/²⁵⁹Cf/²⁶⁰Cf/²⁶¹Cf/²⁶²Cf/²⁶³Cf/²⁴¹Es/²⁴²Es/²⁴³Es/²⁴⁴Es/²⁴⁵Es/²⁴⁶Es/²⁴⁷Es/²⁴⁸Es/²⁴⁹Es/²⁵⁰Es/²⁵¹Es/²⁵²Es/²⁵³Es/²⁵⁴Es/²⁵⁵Es/²⁵⁶Es/²⁵⁷Es/²⁵⁸Es/²⁵⁹Es/²⁶⁰Es/²⁶¹Es/²⁶²Es/²⁶³Es/²⁶⁴Es/²⁴⁸Fm/²⁴⁹Fm/²⁵⁰Fm/²⁵¹Fm/²⁵²Fm/²⁵³Fm/²⁵⁴Fm/²⁵⁵Fm/²⁵⁶Fm/²⁵⁷Fm/²⁵⁸Fm/²⁵⁹Fm/²⁶⁰Fm/²⁶¹Fm/²⁶²Fm/²⁶³Fm/²⁶⁴Fm/²⁶⁵Fm/²⁶⁶Fm/²⁶⁷Fm/²⁵⁰Md/²⁵¹Md/²⁵²Md/²⁵³Md/²⁵⁴Md/²⁵⁵Md/²⁵⁶Md/²⁵⁷Md/²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md/²⁶⁴Md/²⁶⁵Md/²⁶⁶Md, E(cm)=898.71 MeV; calculated primary and final fragments σ(E). ²³⁸U, ²⁴⁴Pu, ²⁴⁸Cm, ²⁴⁹Cf(²²O, 2n), (²²O, 3n), (²²O, 4n), (²²O, 5n), (²²O, 6n), E^*=24-60 MeV; calculated evaporation residue σ(E). ²⁴⁸Cm(²³⁸U, X)²⁴⁶Fm/²⁴⁷Fm/²⁴⁸Fm/²⁴⁹Fm/²⁵⁰Fm/²⁵¹Fm/²⁵²Fm/²⁵³Fm/²⁵⁴Fm/²⁵⁵Fm/²⁵⁶Fm/²⁵⁷Fm/²⁵⁸Fm/²⁵⁹Fm/²⁶⁰Fm/²⁶¹Fm/²⁶²Fm/²⁶³Fm/²⁶⁴Fm/²⁶⁵Fm/²⁵³No/²⁵⁴No/²⁵⁵No/²⁵⁶No/²⁵⁷No/²⁵⁸No/²⁵⁹No/²⁶⁰No/²⁶¹No/²⁶²No/²⁶³No/²⁶⁴No/²⁶⁵No/²⁶⁶No/²⁶⁷No/²⁵⁸Rf/²⁵⁹Rf/²⁶⁰Rf/²⁶¹Rf/²⁶²Rf/²⁶³Rf/²⁶⁴Rf/²⁶⁵Rf/²⁶⁶Rf/²⁶⁷Rf/²⁶⁸Rf/²⁶⁹Rf/²⁶⁵Sg/²⁶⁶Sg/²⁶⁷Sg/²⁶⁸Sg, E(cm)=898.71 MeV; calculated σ(E) of the multinucleon transfer reaction, fusion σ(E). Dinuclear system model (DNS) combined with GEMINI++ for calculating the evaporation residue cross section. Comparison to experimental data.

doi: 10.1103/PhysRevC.108.024602
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2022ZH13      Nucl.Phys. A1021, 122420 (2022)

T.Zhao, H.Zhang

A new method to improve the generalization ability of neural networks: A case study of nuclear mass training

doi: 10.1016/j.nuclphysa.2022.122420
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2022ZH38      Chin.Phys.C 46, 044103 (2022)

T.-L.Zhao, H.-F.Zhang

A neural network approach based on more input neurons to predict nuclear mass

NUCLEAR STRUCTURE Z=1-118; calculated atomic masses using the neural network (NN) approach. Comparison with available data.

doi: 10.1088/1674-1137/ac3e5b
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2022ZH47      Nucl.Phys. A1027, 122510 (2022)

T.L.Zhao, X.J.Bao, H.F.Zhang

Improvement of evaporation residual cross sections for superheavy nuclei using a neural network method

NUCLEAR REACTIONS ²⁴⁸Cm(¹⁸O, X), ^242,244Pu(²²Ne, X), ²³⁸U(²⁶Mg, X), ²⁴⁹Cf(¹⁵N, X), ²⁴⁹Bk(¹⁶O, X), ²⁴⁸Cm(¹⁹F, X), ²⁴¹Am(²²Ne, X), ²³⁸U(³⁰Si, X), ²⁴⁹Cf(¹⁸O, X), ²⁴⁸Cm(²²Ne, X), ²⁴⁹Bk(²²Ne, X), ²⁴⁸Cm(²⁶Mg, X), ²³⁸U(³⁶S, X), (³⁴S, X), ²²⁶Ra(⁴⁸Ca, X), ²³²Th(⁴⁸Ca, X), ²³⁸U(⁴⁸Ca, X), ²³⁷Np(⁴⁸Ca, X), ^{239,240,242,244}Pu(⁴⁸Ca, X), ²⁴³Am(⁴⁸Ca, X), ^245,248Cm(⁴⁸Ca, X), ²⁴⁹Bk(⁴⁸Ca, X), ²⁴⁹Cf(⁴⁸Ca, X)Rf/Db/Sg/Bh/Ds/Hs/Nh/Cn/Fl/Mc/Lv/Ts/Og, E not given; calculated evaporation residual cross section (ERCS) using the neural network method. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122510
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2022ZH55      J.Phys.(London) G49, 105104 (2022)

T.L.Zhao, H.F.Zhang

Unified description of α decay and cluster radioactivity using the neural network approach and universal decay law

RADIOACTIVITY ²⁵⁶Fm(⁴⁶Ar), (⁴⁸Ar), (⁴⁸Ca), (⁵⁰Ca), (⁵²Ca), ²⁵²No(⁴⁴Ar), ²⁵⁴No(⁴⁴Ar), (⁴⁶Ar), (⁴⁸Ca), ²⁵⁶No(⁴⁴Ar), (⁴⁶Ar), (⁴⁸Ar), (⁴⁸Ca), (⁵⁰Ca), ^240,242Cf(³⁰Si), (³²Si), ²⁴²Cf(³⁴Si), (³⁶S), ²⁴⁴Cf(³²Si), (³⁴Si), (³⁶S), (³⁸Si), ²⁴⁶Cf(³⁴Si), (³⁶S), (³⁸Si), (⁴⁰Si), ²⁴⁸Cf(³⁸Si), (⁴⁰S), (⁴²S), (⁴⁴Ar), ²⁵⁰Cf(⁴⁰S), (⁴²S), (⁴⁴Ar), (⁴⁶Ar), ²⁵²Cf(⁴²S), (⁴⁴Ar), (⁴⁶Ar), (⁴⁸Ar), ²⁵⁴Cf(⁴⁶Ar), (⁴⁸Ar), ²⁵⁴Cf(⁴⁶Ar), (⁴⁸Ar), ^246,248Fm(³⁶S), (³⁸S), ²⁴⁸Fm(⁴⁰S), ²⁵⁰Fm(³⁸S), (⁴⁰S), (⁴²S), (⁴⁴Ar), ²⁵²Fm(⁴⁰S), (⁴²S), (⁴⁴Ar), (⁴⁶Ar), (⁴⁸Ca), ²⁵⁴Fm(⁴²S), (⁴⁴Ar), (⁴⁶Ar), (⁴⁸Ca), (⁵⁰Ca); calculated cluster radioactivity T_1/2 using three UDL formulas as well as two neural network methods.

doi: 10.1088/1361-6471/ac8b26
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2021DR02      Phys.Rev. C 103, 045808 (2021)

C.Drischler, S.Han, J.M.Lattimer, M.Prakash, S.Reddy, T.Zhao

Limiting masses and radii of neutron stars and their implications

doi: 10.1103/PhysRevC.103.045808
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2019XU09      Phys.Rev. C 99, 064303 (2019)

X.Xu, M.Wang, K.Blaum, J.D.Holt, Yu.A.Litvinov, A.Schwenk, J.Simonis, S.R.Stroberg, Y.H.Zhang, H.S.Xu, P.Shuai, X.L.Tu, X.H.Zhou, F.R.Xu, G.Audi, R.J.Chen, X.C.Chen, C.Y.Fu, Z.Ge, W.J.Huang, S.Litvinov, D.W.Liu, Y.H.Lam, X.W.Ma, R.S.Mao, A.Ozawa, B.H.Sun, Y.Sun, T.Uesaka, G.Q.Xiao, Y.M.Xing, T.Yamaguchi, Y.Yamaguchi, X.L.Yan, Q.Zeng, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan

Masses of neutron-rich ^52-54Sc and ^{54, 56}Ti nuclides: The N=32 subshell closure in scandium

ATOMIC MASSES ^52,53,54Sc, ^54,56Ti; measured mass excesses using isochronous mass spectrometry at CRSe-HIRFL, Lanzhou. Isotopes produced in ⁹Be(⁸⁶Kr, X), E=460.65 MeV/nucleon reaction and separated using RIBLL2. Comparison with AME-2012 evaluation, and results from six previous experiments, and with valence-space in-medium similarity renormalization group (VS-IMSRG) calculations. Systematics of S(2n) values in N=27-34 K, Ca, Sc, Ti isotopic chains, and those of empirical shell gaps in N=24-34 K, Ca, Sc, Ti isotopic chains and Z=19-25 N=32 isotones.

doi: 10.1103/PhysRevC.99.064303
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2018ZH03      J.Phys.(London) G45, 025106 (2018)

T.L.Zhao, X.J.Bao, S.Q.Guo

The predictive accuracy of analytical formulas and semiclassical approaches for α decay half-lives of superheavy nuclei

RADIOACTIVITY ^{255,257,259,261}Rf, ^{256,257,258,259,260,261,262,263}Db, ^{259,260,261,263,265,266,271}Sg, ^{261,262,264,266,267,272,274}Bh, ^{264,265,266,267,268,269,270,275}Hs, ^{266,268,270,275,276,278}Mt, ^{267,269,270,271,273,279,281}Ds, ^{272,274,279,280,282}Rg, ^277,283,285Cn, ^{278,283,284,285,286}Nh, ^{286,287,288,289}Fl, ^{287,288,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1088/1361-6471/aa9fbe
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2018ZH58      Phys.Rev. C 98, 064307 (2018)

T.L.Zhao, X.J.Bao

Predictions for decay modes for superheavy nuclei Z=118 - 124

RADIOACTIVITY ²⁹⁴Og, ^293,294Ts, ^{290,291,292,293}Lv, ^{287,288,289,290}Mc, ^{285,286,287,288,289}Fl, ^{282,283,284,285,286}Nh, ^{281,282,283,284,285}Cn, ^{278,279,280,281,282}Rg, ^277,279,281Ds, ^{274,275,276,277,278}Mt, ^273,275,277Hs, ^{270,271,272,274}Bh, ^269,271Sg, ^{266,267,268,270}Db, ^265,267Rf, ^{301,302,303,304,305,306,307,308,309,310,311,312}124, ^{300,301,302,303,304,305,306,307,308,309,310,311}123, ^{295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310}122, ^{294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309}121, ^{289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308}120, ^{288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307}119, ^{283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306}Og, ^{288,289,290,291,292,293,294,295,296,297,298,299}Ts, ^{285,286,287,288,289,290,291,292,293,294,295,296}Lv, ^{284,285,286,287,288,289,290,291,292,293,294,295}Mc, ^{281,282,283,284,285,286,287,288,289,290,291,292}Fl, ^{280,281,282,283,284,285,286,287,288,289,290,291}Nh, ^{277,278,279,280,281,282,283,284,285,286,287,288}Cn, ^{276,277,278,279,280,281,282,283,284,285,286,287}Rg, ^{273,274,275,276,277,278,279,280,281,282,283,284}Ds, ^{272,273,274,275,276,277,278,279,280,281,282,283}Mt, ^{269,270,271,272,273,274,275,276,277,278,279,280}Hs, ^{268,269,270,271,272,273,274,275,276,277,278,279}Bh, ^{265,266,267,268,269,270,271,272,273,274,275,276}Sg, ^{264,265,266,267,268,269,270,271,272,273,274}Db, ^{261,262,263,264,265,266,267,268,269,270,271,272}Rf(α), (SF); calculated half-lives, and (α/SF) decay modes using a generalized liquid drop model (GLDM) with universal decay law (UDL) for α decay, and generalized Swiatecki's formulas (Bao, KPS and NAVK) for SF decay. Comparison with available experimental values.

doi: 10.1103/PhysRevC.98.064307
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2017TU01      Phys.Rev. C 95, 014610 (2017)

X.L.Tu, A.Kelic-Heil, Yu.A.Litvinov, Zs.Podolyak, Y.H.Zhang, W.J.Huang, H.S.Xu, K.Blaum, F.Bosch, R.J.Chen, X.C.Chen, C.Y.Fu, B.S.Gao, Z.Ge, Z.G.Hu, D.W.Liu, S.A.Litvinov, X.W.Ma, R.S.Mao, B.Mei, P.Shuai, B.H.Sun, Y.Sun, Z.Y.Sun, P.M.Walker, M.Wang, N.Winckler, J.W.Xia, G.Q.Xiao, Y.M.Xing, X.Xu, T.Yamaguchi, X.L.Yan, J.C.Yang, Y.J.Yuan, Q.Zeng, W.Zhang, H.W.Zhao, T.C.Zhao, X.H.Zhou

Application of isochronous mass spectrometry for the study of angular momentum population in projectile fragmentation reactions

NUCLEAR REACTIONS ⁹Be(⁷⁸Kr, X)⁵³Fe/^53mFe/⁵³Co/^53mCo, E=479.4 MeV/nucleon; measured revolution time spectra of the isomeric and ground states of ⁵³Co and ⁵³Fe using isochronous mass spectrometry (IMS) technique at HIRFL-CSR-Lanzhou facility; deduced isomeric ratios for the 19/2 state, and compared with the predictions of theoretical calculations using ABRABLA07 code. ⁵³Fe; calculated production probability of ⁵³Fe versus spin using ABRABLA07 code for the ⁵⁸Ni, ⁷⁸Kr, ⁸⁴Kr, and ¹¹²Sn projectiles.

doi: 10.1103/PhysRevC.95.014610
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2015XU14      Chin.Phys.C 39, 104001 (2015)

X.Xu, M.Wang, Y.-H.Zhang, H.-S.Xu, P.Shuai, X.-L.Tu, Y.A.Litvinov, X.-H.Zhou, B.-H.Sun, Y.-J.Yuan, J.-W.Xia, J.-C.Yang, K.Blaum, R.-J.Chen, X.-C.Chen, C.-Y.Fu, Z.Ge, Z.-G.Hu, W.-J.Huang, D.-W.Liu, Y.-H.Lam, X.-W.Ma, R.-S.Mao, T.Uesaka, G.-Q.Xiao, Y.-M.Xing, T.Yamaguchi, Y.Yamaguchi, Q.Zeng, X.-L.Yan, H.-W.Zhao, T.-C.Zhao, W.Zhang, W.-L.Zhan

Direct mass measurements of neutron-rich ⁸⁶Kr projectile fragments and the persistence of neutron magic number N=32 in Sc isotopes

ATOMIC MASSES ²³F, ²⁵Ne, ³³Al, ³⁶Si, ³⁸P, ^42,43Cl, ^52,53,54Sc, ^54,56Ti, ^57,58V, ⁶¹Cr, ⁶⁹Co; measured corrected revolution time spectrum; deduced mass excess values. Comparison with AME12 mass evaluation.

doi: 10.1088/1674-1137/39/10/104001
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2014SH14      Phys.Lett. B 735, 327 (2014)

P.Shuai, H.S.Xu, X.L.Tu, Y.H.Zhang, B.H.Sun, M.Wang, Yu.A.Litvinov, K.Blaum, X.H.Zhou, J.J.He, Y.Sun, K.Kaneko, Y.J.Yuan, J.W.Xia, J.C.Yang, G.Audi, X.L.Yan, X.C.Chen, G.B.Jia, Z.G.Hu, X.W.Ma, R.S.Mao, B.Mei, Z.Y.Sun, S.T.Wang, G.Q.Xiao, X.Xu, T.Yamaguchi, Y.Yamaguchi, Y.D.Zang, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan

Charge and frequency resolved isochronous mass spectrometry and the mass of ⁵¹Co

ATOMIC MASSES ⁵¹Co, ³⁴Ar; measured revolution frequencies; deduced mass excess values. Comparison with shell model calculations.

doi: 10.1016/j.physletb.2014.06.046
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2013YA03      Astrophys.J. 766, L8 (2013)

X.L.Yan, H.S.Xu, Yu.A.Litvinov, Y.H.Zhang, H.Schatz, X.L.Tu, K.Blaum, X.H.Zhou, B.H.Sun, J.J.He, Y.Sun, M.Wang, Y.J.Yuan, J.W.Xia, J.C.Yang, G.Audi, G.B.Jia, Z.G.Hu, X.W.Ma, R.S.Mao, B.Mei, P.Shuai, Z.Y.Sun, S.T.Wang, G.Q.Xiao, X.XU, T.Yamaguchi, Y.Yamaguchi, Y.D.Zang, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan

Mass Measurement of ⁴⁵Cr and Its Impact on the Ca-Sc Cycle in X-Ray Bursts

ATOMIC MASSES ⁴¹Ti, ⁴³V, ⁴⁵Cr, ⁴⁷Mn, ⁴⁹Fe, ⁵³Ni, ⁵⁵Cu; measured revolution frequencies; deduced masses. Comparison with available data.

doi: 10.1088/2041-8205/766/1/L8
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2012ZH06      Phys.Rev. C 85, 024621 (2012)

X.H.Zhang, Z.Y.Sun, R.F.Chen, Z.Q.Chen, Z.Y.Guo, J.L.Han, Z.G.Hu, T.H.Huang, R.S.Mao, Z.G.Xu, M.Wang, J.S.Wang, Y.Wang, G.Q.Xiao, H.S.Xu, X.H.Yuan, H.B.Zhang, X.Y.Zhang, T.C.Zhao

Projectile fragmentation reactions of ⁴⁰Ar at 57 MeV/nucleon

NUCLEAR REACTIONS ⁹Be(⁴⁰Ar, X)¹⁷F/¹⁸F/¹⁹F/²⁰F/²¹F/²²F/²³F/²⁴F/²⁵F/¹⁹Ne/²⁰Ne/²¹Ne/²²Ne/²³Ne/²⁴Ne/²⁵Ne/²⁶Ne/²⁷Ne/²¹Na/²²Na/²³Na/²⁴Na/²⁵Na/²⁶Na/²⁷Na/²⁸Na/²⁹Na/³⁰Na/²²Mg/²³Mg/²⁴Mg/²⁵Mg/²⁶Mg/²⁷Mg/²⁸Mg/²⁹Mg/³⁰Mg/³¹Mg/³²Mg/²⁴Al/²⁵Al/²⁶Al/²⁷Al/²⁸Al/²⁹Al/³⁰Al/³¹Al/³²Al/³³Al/³⁴Al/³⁵Al/²⁶Si/²⁷Si/²⁸Si/²⁹Si/³⁰Si/³¹Si/³²Si/³³Si/³⁴Si/³⁵Si/³⁶Si/³⁷Si/²⁸P/²⁹P/³⁰P/³¹P/³²P/³³P/³⁴P/³⁵P/³⁶P/³⁷P/³⁸P/³⁹P/³⁰S/³¹S/³²S/³³S/³⁴S/³⁵S/³⁶S/³⁷S/³⁸S/³⁹S/⁴⁰S/³²Cl/³³Cl/³⁴Cl/³⁵Cl/³⁶Cl/³⁷Cl/³⁸Cl/³⁹Cl/⁴⁰Cl/⁴¹Cl/³⁴Ar/³⁵Ar/³⁶Ar/³⁷Ar/³⁸Ar/³⁹Ar/⁴⁰Ar/⁴¹Ar/⁴¹Ar/³⁷K/³⁸K/³⁹K/⁴⁰K/³⁹Ca/⁴⁰Ca/⁴¹Ca/⁴²Ca, E=57 MeV/nucleon; ¹⁸¹Ta(⁴⁰Ar, X)¹⁷F/¹⁸F/¹⁹F/²⁰F/²¹F/²²F/²³F/²⁴F/²⁵F/¹⁹Ne/²⁰Ne/²¹Ne/²²Ne/²³Ne/²⁴Ne/²⁵Ne/²⁶Ne/²⁷Ne, ²¹Na/²²Na/²³Na/²⁴Na/²⁵Na/²⁶Na/²⁷Na/²⁸Na/²⁹Na/³⁰Na/²³Mg/²⁴Mg/²⁵Mg/²⁶Mg/²⁷Mg/²⁸Mg/²⁹Mg/³⁰Mg/³¹Mg/³²Mg/²⁵Al/²⁶Al/²⁷Al/²⁸Al/²⁹Al/³⁰Al/³¹Al/³²Al/³³Al/³⁴Al/, ²⁷Si/²⁸Si/²⁹Si/³⁰Si/³¹Si/³²Si/³³Si/³⁴Si/³⁵Si/³⁶Si/²⁹P/³⁰P/³¹P/³²P/³³P/³⁴P/³⁵P/³⁶P/³⁷P/³⁸P/³¹S/³²S/³³S/³⁴S/³⁵S/³⁶S/³⁷S/³⁸S/³⁹S/⁴⁰S/³³Cl/³⁴Cl/³⁵Cl/³⁶Cl/³⁷Cl/³⁸Cl/³⁹Cl/⁴⁰Cl/³⁵Ar/³⁶Ar/³⁷Ar/³⁸Ar/³⁹Ar/³⁸K/³⁹K/⁴⁰K/⁴⁰Ca/⁴¹Ca, E=57 MeV/nucleon; measured particle spectra, energy loss, time of flight, fragment yields, momentum distributions, cross sections; deduced fragment excitation energies, mass yield ratios. RIBLL, HIRFL facilities. Comparison with empirical parameterization of fragmentation cross section (EPAX), abrasion-ablation (AA) model, and heavy-ion phase-space exploration (HIPSE) model. Discussed target dependence of fragment cross sections.

doi: 10.1103/PhysRevC.85.024621
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2012ZH34      Phys.Rev.Lett. 109, 102501 (2012)

Y.H.Zhang, H.S.Xu, Yu.A.Litvinov, X.L.Tu, X.L.Yan, S.Typel, K.Blaum, M.Wang, X.H.Zhou, Y.Sun, B.A.Brown, Y.J.Yuan, J.W.Xia, J.C.Yang, G.Audi, X.C.Chen, G.B.Jia, Z.G.Hu, X.W.Ma, R.S.Mao, B.Mei, P.Shuai, Z.Y.Sun, S.T.Wang, G.Q.Xiao, X.Xu, T.Yamaguchi, Y.Yamaguchi, Y.D.Zang, H.W.Zhao, T.C.Zhao, W.Zhang, W.L.Zhan

Mass Measurements of the Neutron-Deficient ⁴¹Ti, ⁴⁵Cr, ⁴⁹Fe, and ⁵³Ni Nuclides: First Test of the Isobaric Multiplet Mass Equation in fp-Shell Nuclei

ATOMIC MASSES ⁴¹Ti, ⁴⁵Cr, ⁴⁹Fe, ⁵³Ni; measured ion revolution time; deduced mass excess values, test for the isobaric multiplet mass equation in fp-shell nuclei. Shell model calculation, comparison with available data.

doi: 10.1103/PhysRevLett.109.102501
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2011TU02      Phys.Rev.Lett. 106, 112501 (2011)

X.L.Tu, H.S.Xu M.Wang, Y.H.Zhang, Yu.A.Litvinov, Y.Sun, H.Schatz, X.H.Zhou, Y.J.Yuan, J.W.Xia, G.Audi, K.Blaum, C.M.Du, P.Geng, Z.G.Hu, W.X.Huang, S.L.Jin, L.X.Liu, Y.Liu, X.Ma, R.S.Mao, B.Mei, P.Shuai, Z.Y.Sun, H.Suzuki, S.W.Tang, J.S.Wang, S.T.Wang, G.Q.Xiao, X.Xu, T.Yamaguchi, Y.Yamaguchi, X.L.Yan, J.C.Yang, R.P.Ye, Y.D.Zang, H.W.Zhao, T.C.Zhao, X.Y.Zhang, W.L.Zhan

Direct Mass Measurements of Short-Lived A=2Z-1 Nuclides ⁶³Ge, ⁶⁵As, ⁶⁷Se, and ⁷¹Kr and Their Impact on Nucleosynthesis in the rp Process

ATOMIC MASSES ⁶³Ge, ⁶⁵As, ⁶⁷Se, ⁷¹Kr; measured ion time resolution; deduced mass excesses, proton separation energy. Comparison with AME03 and mirror nuclei, x-ray luminosity and mass number abundances calculations.

doi: 10.1103/PhysRevLett.106.112501
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2011TU09      Nucl.Instrum.Methods Phys.Res. A654, 213 (2011)

X.L.Tu, M.Wang, Yu.A.Litvinov, Y.H.Zhang, H.S.Xu, Z.Y.Sun, G.Audi, K.Blaum, C.M.Du, W.X.Huang, Z.G.Hu, P.Geng, S.L.Jin, L.X.Liu, Y.Liu, B.Mei, R.S.Mao, X.W.Ma, H.Suzuki, P.Shuai, Y.Sun, S.W.Tang, J.S.Wang, S.T.Wang, G.Q.Xiao, X.Xu, J.W.Xia, J.C.Yang, R.P.Ye, T.Yamaguchi, X.L.Yan, Y.J.Yuan, Y.Yamaguchi, Y.D.Zang, H.W.Zhao, T.C.Zhao, X.Y.Zhang, X.H.Zhou, W.L.Zhan

Precision isochronous mass measurements at the storage ring CSRe in Lanzhou

ATOMIC MASSES ³³Cl, ³⁵Ar, ³⁷K, ³⁹Ca, ⁴¹Sc, ⁴⁵V, ⁴⁷Cr, ⁴⁹Mn, ⁵¹Fe, ⁵³Co, ⁵⁵Ni, ⁵⁷Cu, ⁵⁹Zn, ⁶¹Ga; measured revolution time spectra; deduced mass excess values. Comparison with available data.

doi: 10.1016/j.nima.2011.07.018
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2009WA05      Int.J.Mod.Phys. E18, 352 (2009)

M.Wang, H.S.Xu, J.W.Xia, X.L.Tu, R.S.Mao, Y.J.Yuan, Z.G.Hu, Y.Liu, H.B.Zhang, Y.D.Zang, T.C.Zhao, X.Y.Zhang, F.Fu, J.C.Yang, L.J.Mao, C.Xiao, G.Q.Xiao, H.W.Zhao, W.L.Zhan

First isochronous mass measurements at CSRe

doi: 10.1142/S0218301309012380
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2006WA17      Chin.Phys.Lett. 23, 1731 (2006)

Q.Wang, J.-L.Han, Z.-G.Xiao, H.-S.Xu, Z.-Yu.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X.-H.Yuan, Z.-G.Xu, T.-C.Zhao, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, Z.Bai, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, Yu.-K.Sergey

Exotic Behaviour of Angular Dispersion of Weakly Bound Nucleus ¹⁷F at Small Angles

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷F, ¹⁷F), E=141 MeV; ²⁰⁸Pb(¹⁷O, ¹⁷O), E=128 MeV; measured σ(θ); deduced possible halo effects.

doi: 10.1088/0256-307X/23/7/021
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2004MO27      Nucl.Phys. A738, 129 (2004)

K.Morimoto, K.Morita, D.Kaji, S.Goto, H.Haba, E.Ideguchi, R.Kanungo, K.Katori, H.Koura, H.Kudo, T.Ohnishi, A.Ozawa, J.C.Peter, T.Suda, K.Sueki, I.Tanihata, F.Tokanai, H.Xu, A.V.Yeremin, A.Yoneda, A.Yoshida, T.-L.Zhao, T.Zheng

Status of super heavy element research using GARIS at RIKEN

NUCLEAR REACTIONS ²⁰⁸Pb, ²⁰⁹Bi(⁶⁴Ni, n), E=310-326 MeV; measured excitation functions.

RADIOACTIVITY ²⁷¹Ds, ²⁶⁷Hs, ²⁶³Sg, ²⁵⁹Rf, ²⁵⁵No(α) [from ²⁰⁸Pb(⁶⁴Ni, n) and subsequent decay]; ²⁷²Rg, ²⁶⁸Mt, ²⁶⁴Bh, ²⁶⁰Db, ²⁵⁶Lr(α) [from ²⁰⁹Bi(⁶⁴Ni, n) and subsequent decay]; measured Eα, T_1/2.

doi: 10.1016/j.nuclphysa.2004.04.021
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Note: The following list of authors and aliases matches the search parameter T.Zhao: , T.C.ZHAO, T.L.ZHAO